Determinants and Their Applications in Mathematical Physics

(Chris Devlin) #1

308 Appendix


and letInandJndenote arrangements or permutations of the samen


integers


In=

{

i 1 i 2 i 3 ···in

}

,

Jn=

{

j 1 j 2 j 3 ···jn

}

.

There aren! possible sets of the formInorJnincludingNn. The num-


bers within the set are called elements. The operation which consists of


interchanging any two elements in a set is called an inversion. Assuming


thatJn=In, that is,jr=irfor at least two values ofr, it is possible to


transformJnintoInby means of a sequence of inversions. For example, it


is possible to transform the set{ 35214 }into the setN 5 in four steps,


that is, by means of four inversions, as follows:


35214

1: 15234

2: 12534

3: 12354

4: 12345

The choice of inversions is clearly not unique for the transformation can


also be accomplished as follows:


35214

1: 34215

2: 31245

3: 21345

4: 12345

No steps have been wasted in either method, that is, the methods are


efficient and several other efficient methods can be found. If steps are wasted


by, for example, removing an element from its final position at any stage


of the transformation, then the number of inversions required to complete


the transformation is increased.


However, it is known that if the number of inversions required to trans-

formJnintoInis odd by one method, then it is odd by all methods, and


Jnis said to be an odd permutation ofIn. Similarly, if the number of in-


versions required to transformJnintoInis even by one method, then it is


even by all methods, andJnis said to be an even permutation ofIn.


The permutation symbol is an expression of the form

{
In

Jn

}

=

{

i 1 i 2 i 3 ··· in

j 1 j 2 j 3 ··· jn

}

,

which enablesInto be compared withJn.


The sign of the permutation symbol, denoted byσ, is defined as follows:

σ= sgn

{

In

Jn

}

= sgn

{

i 1 i 2 i 3 ··· in

j 1 j 2 j 3 ··· jn

}

=(−1)

m
,
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